CN109520532B - A multi-sensor multiplexing demodulation system and processing method of a fiber optic Faber sensor - Google Patents
A multi-sensor multiplexing demodulation system and processing method of a fiber optic Faber sensor Download PDFInfo
- Publication number
- CN109520532B CN109520532B CN201811419299.9A CN201811419299A CN109520532B CN 109520532 B CN109520532 B CN 109520532B CN 201811419299 A CN201811419299 A CN 201811419299A CN 109520532 B CN109520532 B CN 109520532B
- Authority
- CN
- China
- Prior art keywords
- sensor
- spectrum
- frequency
- interference
- optical fiber
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Active
Links
- 239000000835 fiber Substances 0.000 title claims abstract description 38
- 238000003672 processing method Methods 0.000 title claims abstract description 6
- CRQQGFGUEAVUIL-UHFFFAOYSA-N chlorothalonil Chemical compound ClC1=C(Cl)C(C#N)=C(Cl)C(C#N)=C1Cl CRQQGFGUEAVUIL-UHFFFAOYSA-N 0.000 title abstract description 4
- 230000003595 spectral effect Effects 0.000 claims abstract description 47
- 238000001228 spectrum Methods 0.000 claims abstract description 41
- 239000013307 optical fiber Substances 0.000 claims abstract description 20
- 230000003287 optical effect Effects 0.000 claims abstract description 14
- 238000001514 detection method Methods 0.000 claims abstract description 13
- 238000000034 method Methods 0.000 claims abstract description 13
- 238000005070 sampling Methods 0.000 claims abstract description 8
- 230000003321 amplification Effects 0.000 claims description 4
- 238000003199 nucleic acid amplification method Methods 0.000 claims description 4
- 238000010408 sweeping Methods 0.000 claims 1
- 238000010586 diagram Methods 0.000 description 9
- 238000005259 measurement Methods 0.000 description 8
- 238000004364 calculation method Methods 0.000 description 5
- 238000004891 communication Methods 0.000 description 4
- 230000009286 beneficial effect Effects 0.000 description 2
- 230000001427 coherent effect Effects 0.000 description 2
- 238000005516 engineering process Methods 0.000 description 2
- 229910000530 Gallium indium arsenide Inorganic materials 0.000 description 1
- KXNLCSXBJCPWGL-UHFFFAOYSA-N [Ga].[As].[In] Chemical compound [Ga].[As].[In] KXNLCSXBJCPWGL-UHFFFAOYSA-N 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 239000003245 coal Substances 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 239000002360 explosive Substances 0.000 description 1
- 229910052732 germanium Inorganic materials 0.000 description 1
- GNPVGFCGXDBREM-UHFFFAOYSA-N germanium atom Chemical compound [Ge] GNPVGFCGXDBREM-UHFFFAOYSA-N 0.000 description 1
- 238000005305 interferometry Methods 0.000 description 1
- 230000007774 longterm Effects 0.000 description 1
- 239000003208 petroleum Substances 0.000 description 1
- 238000010183 spectrum analysis Methods 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
Images
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01D—MEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
- G01D5/00—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
- G01D5/26—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light
- G01D5/268—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light using optical fibres
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01D—MEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
- G01D5/00—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
- G01D5/26—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light
- G01D5/266—Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light by interferometric means
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optical Transform (AREA)
Abstract
本发明涉及一种光纤法珀传感器的多传感器复用解调系统及处理方法,属于光纤传感技术领域。该系统由宽带扫频激光光源、光环形器、波分复用器、光电探测模块、光谱还原模块和数据处理模块依次连接组成,并以并联复用的方式分别连接N个大腔长光纤法珀传感器;该处理方法包括:S1:利用光谱还原模块,将接收到的干涉光谱还原为N段干涉光谱信号;S2:用稀疏采样的频率解调法,对每段光谱数据分别进行处理计算,求出各自的等效频率值;S3:根据等效频率值与光纤法珀传感器的腔长关系,分别求解出N个光纤法珀传感器的值。本发明有效解决了白光干涉型光纤法珀传感器的大容量并联复用难题。
The invention relates to a multi-sensor multiplexing demodulation system and a processing method of an optical fiber Faber sensor, and belongs to the technical field of optical fiber sensing. The system is composed of broadband swept laser light source, optical circulator, wavelength division multiplexer, photoelectric detection module, spectrum restoration module and data processing module connected in sequence, and connected to N large-cavity-length optical fibers in parallel multiplexing mode. The processing method includes: S1: using a spectrum restoration module to restore the received interference spectrum into N-segment interference spectrum signals; S2: using the sparse sampling frequency demodulation method to process and calculate each segment of spectral data separately, Obtain the respective equivalent frequency values; S3: According to the relationship between the equivalent frequency value and the cavity length of the fiber Fa-Per sensor, respectively obtain the values of the N fiber Fa-Per sensors. The invention effectively solves the large-capacity parallel multiplexing problem of the white light interference type optical fiber Fa-Per sensor.
Description
技术领域technical field
本发明属于光纤传感技术领域,涉及一种白光干涉型光纤法珀传感器的多传感器复用解调系统及处理方法。The invention belongs to the technical field of optical fiber sensing, and relates to a multi-sensor multiplexing demodulation system and a processing method of a white light interference type optical fiber Fa-Per sensor.
背景技术Background technique
白光干涉型光纤法珀传感器是一种利用宽光谱干涉实现高精度测量的光纤传感器,它具有传感器体积小、传感器端不带电、抗电磁辐射、耐高温抗腐蚀、易远程传感、与光纤通信兼容等优点。因此在石油、化工、煤矿、机械、以及各种易燃易爆及恶劣工作环境的特殊场合中具有极大的应用潜力。White light interferometric fiber optic sensor is a fiber optic sensor that uses wide spectrum interference to achieve high-precision measurement. Compatibility, etc. Therefore, it has great application potential in special occasions such as petroleum, chemical industry, coal mine, machinery, and various flammable, explosive and harsh working environments.
光纤白光干涉测量系统的典型解调系统原理图2所示,它由低相干宽带光源(11)、光耦合器(12)、光谱仪(13)、数据处理单元(14)组成。若低相干宽带光源具有图3(a)的理想宽带光谱特性,经过传输光纤达到光纤法珀传感器(21)后返回图3(b)的宽光谱干涉信号,该信号经光谱仪采集、再由后续数据处理单元用相应的解调算法进行腔长的计算处理,完成解调。这样的测量系统具有结构简单、技术成熟、易于实现的优点。但其难以实现多传感器复用的缺陷,制约了其大规模的工程应用。Figure 2 shows the typical demodulation system principle of the optical fiber white light interferometry system, which consists of a low-coherence broadband light source (11), an optical coupler (12), a spectrometer (13), and a data processing unit (14). If the low-coherence broadband light source has the ideal broadband spectral characteristics of Fig. 3(a), it will reach the fiber Fa-Per sensor (21) through the transmission fiber and return to the broadband interference signal shown in Fig. 3(b). The data processing unit uses the corresponding demodulation algorithm to calculate and process the cavity length to complete the demodulation. Such a measurement system has the advantages of simple structure, mature technology and easy implementation. However, it is difficult to realize multi-sensor multiplexing, which restricts its large-scale engineering application.
针对白光干涉传感器的多传感器复用问题,目前主要有时分复用与频分复用两种复用技术。时分复用是使用光开关分时地将光源切换到多个传感器并进行解调,虽然它使每个传感器具有相同的解调精度,但光路的切换却限制了系统整体的测量速度,且机械切换结构的长期可靠性较低。频分复用同时获取腔长L不同的数个传感器的干涉光谱信号,再对干涉光谱信号进行频谱分析,利用频谱上的不同峰值将传感器区分出来;由于它要求各个光纤法珀传感器的腔长不同,复用的数量少,实用性差。For the multi-sensor multiplexing problem of white light interferometric sensors, there are mainly two multiplexing technologies: time division multiplexing and frequency division multiplexing. Time division multiplexing uses an optical switch to switch the light source to multiple sensors and demodulate them in time. Although it enables each sensor to have the same demodulation accuracy, the switching of the optical path limits the overall measurement speed of the system, and the mechanical The long-term reliability of the switching structure is low. Frequency division multiplexing obtains the interference spectral signals of several sensors with different cavity lengths L at the same time, and then performs spectrum analysis on the interference spectral signals, and uses different peaks on the spectrum to distinguish the sensors; because it requires the cavity length of each fiber Fa-Per sensor Different, the number of reuse is small, and the practicability is poor.
因此,白光干涉型光纤法珀传感器的多传感器复用,成了制约该类传感器大规模应用的瓶颈之一。Therefore, the multi-sensor multiplexing of white light interferometric fiber optic sensors has become one of the bottlenecks restricting the large-scale application of such sensors.
发明内容SUMMARY OF THE INVENTION
有鉴于此,本发明的目的在于提供一种白光干涉光纤法珀传感器的多传感器复用解调方法与系统,通过使用光谱线宽窄、扫频范围宽的扫频激光光源与大腔长光纤法珀传感器结合的解决方案,并配以与光源波长范围匹配的波分复用器、以及后续稀疏光谱采样解调算法,在不降低相干信号对比度的条件下,有效解决白光干涉型光纤法珀传感器的大容量并联复用难题。In view of this, the purpose of the present invention is to provide a multi-sensor multiplexing demodulation method and system for a white light interference fiber optic sensor. The combined solution of the Perspective sensor, coupled with the wavelength division multiplexer matching the wavelength range of the light source, and the subsequent sparse spectrum sampling and demodulation algorithm, can effectively solve the white light interference type fiber Faber sensor without reducing the contrast of the coherent signal. The large-capacity parallel multiplexing problem.
为达到上述目的,本发明提供如下技术方案:To achieve the above object, the present invention provides the following technical solutions:
一种白光干涉型光纤法珀传感器的多传感器复用解调系统,该系统如图1所示,由扫频激光光源(101)、光环形器(102)、波分复用器(103)、光电探测模块(104)、光谱还原模块(105)和数据处理模块(106)依次连接组成N通道的复用解调系统(1),并分别连接N个大腔长光纤法珀传感器(2);A multi-sensor multiplexing demodulation system of a white light interference type optical fiber Fa-Per sensor, the system is shown in FIG. , a photoelectric detection module (104), a spectrum restoration module (105) and a data processing module (106) are sequentially connected to form an N-channel multiplexing and demodulation system (1), and are respectively connected to N large-cavity-length fiber Fa-Per sensors (2). );
所述扫频激光器的光谱线宽窄、扫频范围宽,以在较宽的光谱范围内输出波长可变的窄线宽扫频激光束;The frequency sweep laser has a narrow spectral line width and a wide frequency sweep range, so as to output a narrow line width sweep frequency laser beam with variable wavelength in a wider spectral range;
所述光环形器用于将扫频激光器发出的扫频激光束单向传递至波分复用器;The optical circulator is used to unidirectionally transmit the swept-frequency laser beam emitted by the swept-frequency laser to the wavelength division multiplexer;
所述波分复用器用于将扫频光谱范围内的激光信号分割为N路窄带光谱信号,并分别传输至N个光纤法珀传感器,再将光纤法珀传感器返回的N路窄带光谱干涉信号合并后、经光环行器传输到光电探测模块;The wavelength division multiplexer is used to divide the laser signal in the swept spectral range into N channels of narrow-band spectral signals, which are respectively transmitted to N fiber Fa-Per sensors, and then the N channels of narrow-band spectral interference signals returned by the fiber Fa-Per sensor are returned. After merging, it is transmitted to the photoelectric detection module through the optical circulator;
所述光电探测模块用于将从N个光纤法珀传感器返回的干涉信号转换为随时间变化的电信号,再经放大、采样转换为离散的数字电信号;The photoelectric detection module is used to convert the interference signals returned from the N fiber Faber sensors into electrical signals that vary with time, and then convert them into discrete digital electrical signals through amplification and sampling;
所述光谱还原模块用于将时域扫描干涉光谱信号转换为光谱波长域的干涉光谱信号;The spectral restoration module is used to convert the time domain scanning interference spectral signal into the interference spectral signal of the spectral wavelength domain;
所述数据处理模块用于将干涉光谱信号,解调计算出N个光纤法珀传感器的腔长值。The data processing module is used for demodulating the interference spectrum signal to calculate the cavity length value of the N fiber Fa-Per sensors.
进一步,所述N个大腔长的光纤法珀传感器,其每个的腔长L都应满足Lmin<L<Lmax,以确保每个传感器都能够产生足够多的干涉条纹数、以满足后续解调计算的要求。Further, each of the N optical fiber Fa-Per sensors with large cavity length should satisfy L min <L<L max , so as to ensure that each sensor can generate enough interference fringes to satisfy Requirements for subsequent demodulation calculations.
所述光纤法珀传感器的腔长上限Lmax及下限Lmin分别满足下二式:The upper limit L max and the lower limit L min of the cavity length of the optical fiber Fa-Per sensor satisfy the following two equations respectively:
其中FMHW为扫频激光的光谱线宽,Δλ与λc分别为扫频激光光源扫频的光谱范围及其中心波长(如图4所示);而波分复用器一个通道的光谱带宽B(如图5(a)所示),其通道数N及频率间隔δf满足下两式:where FMHW is the spectral linewidth of the swept-frequency laser, Δλ and λc are the swept spectral range and the center wavelength of the swept-frequency laser light source respectively (as shown in Figure 4); and the spectral bandwidth B of one channel of the wavelength division multiplexer (as shown in Figure 5(a)), the number of channels N and the frequency interval δf satisfy the following two formulas:
N=Δλ/B (3)N=Δλ/B (3)
进一步,适用于所述解调系统的多传感器处理方法,包括以下步骤:Further, a multi-sensor processing method applicable to the demodulation system includes the following steps:
S1:利用光谱还原模块将接收到的干涉光谱还原为N段干涉光谱信号;S1: Use the spectrum restoration module to restore the received interference spectrum to the N-band interference spectrum signal;
S2:用稀疏采样的频率解调法,对每段光谱数据分别进行处理计算,求出各自的等效频率值;S2: Use the frequency demodulation method of sparse sampling to process and calculate each segment of spectral data separately to obtain their respective equivalent frequency values;
S3:根据等效频率值与光纤法珀传感器的腔长关系,分别求解出N个光纤法珀传感器的值。S3: According to the relationship between the equivalent frequency value and the cavity length of the fiber Fa-Per sensor, the values of N fiber Fa-Per sensors are calculated respectively.
本发明的有益效果在于:本发明通过将光谱线宽窄、扫频范围宽的扫频激光光源与大腔长光纤法珀传感器结合,并配以波分复用器进行N路光谱分割,从而在不降低相干信号对比度的条件下,减小每个传感器所占用的光谱带宽;并采用稀疏采样的频率解调法,对N个光纤法珀传感器的干涉光谱信号进行解调计算,以保障窄带光谱信号的解调精度;从而有效解决白光干涉型光纤法珀传感器的大容量并联复用难题。The beneficial effects of the present invention are as follows: the present invention combines a swept-frequency laser light source with a narrow spectral line width and a wide sweep frequency range with a large-cavity-length fiber Fa-Per sensor, and is equipped with a wavelength division multiplexer to perform N-way spectral division, thereby achieving The spectral bandwidth occupied by each sensor is reduced without reducing the contrast of coherent signals; and the frequency demodulation method of sparse sampling is used to demodulate and calculate the interference spectral signals of N fiber optic sensors to ensure the narrowband spectrum. The demodulation accuracy of the signal; thus effectively solve the large-capacity parallel multiplexing problem of the white light interference type fiber optic sensor.
附图说明Description of drawings
为了使本发明的目的、技术方案和有益效果更加清楚,本发明提供如下附图进行说明:In order to make the purpose, technical solutions and beneficial effects of the present invention clearer, the present invention provides the following drawings for description:
图1为多路复用白光干涉光纤法珀测量系统结构图;Fig. 1 is the structure diagram of the multiplexed white light interference fiber Fabry measurement system;
图2为现有的典型白光干涉法珀传感器解调系统原理图;Fig. 2 is the schematic diagram of the demodulation system of the existing typical white light interferometric method Perspective sensor;
图3为白光干涉型光纤法珀传感器的光谱图,其中图3(a)、图3(b)分别为低相干度光源的理想光谱图、及其相应的光纤法珀传感器输出的干涉光谱图;Figure 3 is a spectrum diagram of a white light interference fiber Fa-Per sensor, in which Figures 3(a) and 3(b) are the ideal spectrum of a low-coherence light source and the corresponding interference spectrum output of the fiber-based Fa-Per sensor. ;
图4为扫频激光光源的光谱示意图;图4(a)为扫频激光器输出窄线宽光谱扫描过程;图4(b)为其扫频光谱范围;Fig. 4 is the spectral schematic diagram of the swept-frequency laser light source; Fig. 4 (a) is the spectral scanning process of the output narrow linewidth of the swept-frequency laser; Fig. 4 (b) is its swept-frequency spectral range;
图5为本方法干涉信号的复用原理图;图5(a)为N路波分复用器的光谱特性图;图5(b)为这N路光纤法珀传感器各自的干涉光谱图;Figure 5 is a schematic diagram of the multiplexing of interference signals in this method; Figure 5 (a) is a spectral characteristic diagram of an N-way wavelength division multiplexer; Figure 5 (b) is a respective interference spectrum diagram of the N-way optical fiber Fa-Per sensor;
图6为传感器复用光谱的解调算法原理流程框图;Fig. 6 is the principle flow chart of the demodulation algorithm of sensor multiplexing spectrum;
图7为实施例一所述并联复用光纤法珀测量系统结构图;FIG. 7 is a structural diagram of the parallel multiplexed fiber Fa-Per measurement system according to the first embodiment;
图8为实施例二所述并联复用光纤法珀测量系统结构图。FIG. 8 is a structural diagram of the parallel multiplexed optical fiber Faroese measurement system according to the second embodiment.
具体实施方式Detailed ways
下面将结合附图,对本发明的优选实施例进行详细的描述。The preferred embodiments of the present invention will be described in detail below with reference to the accompanying drawings.
如图1所示,由宽带扫频激光器101、光环形器102、波分复用器103、光电探测模块104、光谱还原模块105和数据处理模块106依次连接组成N通道的复用解调系统1,并连接N个大腔长光纤法珀传感器2;As shown in FIG. 1, a broadband
所述宽带扫频激光器101用于在宽光谱范围内提供波长可变的激光光源;所述光环形器102用于将光源发出的宽谱扫频激光信号单向传递至波分复用器,同时将波分复用器返回的光信号单向传输给光电探测模块;所述波分复用器103用于将宽带光分割为多个波长的N路窄带光,并分别传输至N个长腔长光纤法珀传感器,再将光纤法珀传感器返回的干涉光信号合并后返回光环形器;所述光电探测模块104用于将波长扫描的干涉激光信号转换为随时间变化的电信号,再经放大、采样转换为离散的数字电信号;所述光谱还原模块105用于将时域扫描干涉光谱信号转换为光谱波长域的干涉光谱信号;所述数据处理模块106用于从干涉光谱信号中一次性解调计算出N个光纤传感器的腔长值。The
由扫频激光器提供的宽带光源如图4所示,光源任意时刻输出的均是如图4(a)所示的光谱带宽为FWHM的窄谱线激光,当其随随时间进行扫描时,其最终扫频光谱范围为图4(b)所示。The broadband light source provided by the swept-frequency laser is shown in Figure 4. The output of the light source at any time is a narrow-spectrum laser with a spectral bandwidth of FWHM as shown in Figure 4(a). When it scans with time, its The final swept spectral range is shown in Figure 4(b).
波分复用器的光谱特性如图5(a)所示,一个滤波通道相当于一个光谱窄带滤波器,其将一个波长的光输出到对应的端口,并连接一只光纤法珀传感器,从而获得如图5(b)所示多路复用干涉光谱。The spectral characteristics of the wavelength division multiplexer are shown in Figure 5(a), a filter channel is equivalent to a spectral narrowband filter, which outputs a wavelength of light to the corresponding port, and is connected to a fiber optic Fa-Per sensor, thus The multiplexed interference spectrum is obtained as shown in Fig. 5(b).
解调算法包含三步,如图6所示:首先对光谱进行N段分割,再采用稀疏光谱的频率解调算法对各段干涉光谱信号分别进行解调计算,得到N个光纤法珀传感器各自的等效角频率,最后将其转换为光纤法珀传感器腔长,从而完成N个光纤法珀传感器的腔长解调。The demodulation algorithm consists of three steps, as shown in Figure 6: First, the spectrum is divided into N segments, and then the frequency demodulation algorithm of the sparse spectrum is used to demodulate and calculate the interference spectrum signals of each segment respectively, so as to obtain the respective N fiber Fa-Per sensors. The equivalent angular frequency is finally converted into the cavity length of the fiber Fa-Per sensor, thereby completing the cavity length demodulation of N fiber Fa-Per sensors.
为了保证干涉信号的信噪比,N光纤法珀传感器皆采用大腔长的法珀传感器。In order to ensure the signal-to-noise ratio of the interference signal, the N-fiber Fa-Per sensor adopts a Fa-Per sensor with a large cavity length.
所述N个大腔长的光纤法珀传感器,其每个的腔长L都应满足Lmin<L<Lmax,以确保每个传感器都能够产生足够多的干涉条纹数、以满足后续解调计算的要求。For the N fiber-optic Fa-Per sensors with large cavity lengths, each cavity length L should satisfy L min < L < L max , to ensure that each sensor can generate enough interference fringes to satisfy the subsequent solution. Adjustment calculation requirements.
所述光纤法珀传感器的腔长上限Lmax及下限Lmin应分别满足下二式:The upper limit L max and the lower limit L min of the cavity length of the fiber Fa-Per sensor should satisfy the following two equations respectively:
其中FMHW为扫频激光的光谱线宽,Δλ与λc分别为扫频激光光源扫频的光谱范围及其中心波长(如图4所示);而波分复用器一个通道的光谱带宽B(如图5(a)所示),其通道数N及频率间隔δf满足下两式:where FMHW is the spectral linewidth of the swept-frequency laser, Δλ and λc are the swept spectral range and the center wavelength of the swept-frequency laser light source respectively (as shown in Figure 4); and the spectral bandwidth B of one channel of the wavelength division multiplexer (as shown in Figure 5(a)), the number of channels N and the frequency interval δf satisfy the following two formulas:
N=Δλ/B (3)N=Δλ/B (3)
该方法和系统中所涉及的波分复用器、光电探测模块、光谱还原与解调模块及解调算法的实施平台均有多种实现方案。本发明提出两套具体的实施案例:The wavelength division multiplexer, the photoelectric detection module, the spectrum restoration and demodulation module and the implementation platform of the demodulation algorithm involved in the method and system have various implementation schemes. The present invention proposes two sets of specific implementation cases:
1、实施例一1. Example 1
该实施例的系统原理如图7所示,该系统中光源采用通信C波段MEMS型扫频激光器111;波分复用器采用阵列波导光栅型波分复用器(AWG-DWDM)113;光电探测模块由铟镓砷高速光电探测器(InGaAs-PD)114、信号放大电路115和高速ADC采集电路116组成;采用FPGA的光谱还原模块117将信号分割还原成N段干涉光谱信号,并传输至PC机118,由Labview程序实现N个腔长的解调计算。The system principle of this embodiment is shown in FIG. 7 . In this system, the light source adopts a communication C-band MEMS type swept
2、实施例二2.
该实施例的系统原理如图8所示,该系统中光源采用通信C+L波段扫描光栅反馈型扫频激光器121;波分复用器采用体相位全息光栅型密集波分复用器(VPH-DWDM)123,光电探测模块由自带增益的锗高速光电探测器(Ge-APD)124和高速AD采集电路125组成。光谱还原模块采用ARM处理模块126来实现N路光谱的还原;采用高速DSP数据处理系统127进行处理计算,并用嵌入式软件、完成N个腔长的解调计算。The system principle of this embodiment is shown in Figure 8. In this system, the light source adopts the communication C+L band scanning grating feedback type
3、实施效果3. Implementation effect
对图1所示的法珀传感器复用方案,若采用通信C波段带宽为35nm的扫频激光光源和符合国际通信标准G.694.1中通道频率间隔100GHz的波分复用器,光纤法珀传感器的腔长满足公式(1)和公式(2),则可实现40路的光纤法珀传感器多路复用系统,并确保所有干涉传感器之间互相不干扰、独立传感。For the Fa-Per sensor multiplexing scheme shown in Figure 1, if a swept-frequency laser light source with a communication C-band bandwidth of 35nm and a wavelength division multiplexer with a channel frequency interval of 100 GHz in the international communication standard G.694.1 are used, the fiber Fa-Per sensor If the cavity length satisfies formula (1) and formula (2), a 40-channel fiber optic Fa-Per sensor multiplexing system can be realized, and it is ensured that all interference sensors do not interfere with each other and sense independently.
由于一次光谱采集就能获得所有传感器的信息,而系统的测量速度由扫频激光器的光谱扫频速度决定,因此该方案增加传感器复用数并不会降低系统的整体测量速度。故,本发明所述系统采用市售的高速扫频激光器,就对数十上百只光纤传感器达到1kHz以上的复用解调速率。Since the information of all sensors can be obtained in one spectral acquisition, and the measurement speed of the system is determined by the spectral sweep speed of the swept-frequency laser, the increase in the number of multiplexed sensors in this scheme will not reduce the overall measurement speed of the system. Therefore, the system of the present invention uses a commercially available high-speed frequency sweep laser to achieve a multiplexing and demodulation rate of more than 1 kHz for dozens or hundreds of optical fiber sensors.
最后说明的是,以上优选实施例仅用以说明本发明的技术方案而非限制,尽管通过上述优选实施例已经对本发明进行了详细的描述,但本领域技术人员应当理解,可以在形式上和细节上对其作出各种各样的改变,而不偏离本发明权利要求书所限定的范围。Finally, it should be noted that the above preferred embodiments are only used to illustrate the technical solutions of the present invention and not to limit them. Although the present invention has been described in detail through the above preferred embodiments, those skilled in the art should Various changes may be made in details without departing from the scope of the invention as defined by the claims.
Claims (3)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201811419299.9A CN109520532B (en) | 2018-11-26 | 2018-11-26 | A multi-sensor multiplexing demodulation system and processing method of a fiber optic Faber sensor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201811419299.9A CN109520532B (en) | 2018-11-26 | 2018-11-26 | A multi-sensor multiplexing demodulation system and processing method of a fiber optic Faber sensor |
Publications (2)
Publication Number | Publication Date |
---|---|
CN109520532A CN109520532A (en) | 2019-03-26 |
CN109520532B true CN109520532B (en) | 2020-10-16 |
Family
ID=65794290
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201811419299.9A Active CN109520532B (en) | 2018-11-26 | 2018-11-26 | A multi-sensor multiplexing demodulation system and processing method of a fiber optic Faber sensor |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN109520532B (en) |
Families Citing this family (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN110715721A (en) * | 2019-09-12 | 2020-01-21 | 华中科技大学 | FP type acoustic wave sensor multiplexing system and method |
CN110632033B (en) * | 2019-11-08 | 2024-04-12 | 中国计量大学 | Use method of F-P interference type multi-point measurement hydrogen sensor based on FBG demodulator |
CN113607209B (en) * | 2021-06-25 | 2024-11-12 | 重庆大学 | A temperature-strain dual-parameter measurement system based on FBG pairs |
CN115574801B (en) * | 2022-12-09 | 2023-02-24 | 中国船舶集团有限公司第七〇七研究所 | Method for reducing noise based on wavelength division frequency division multiplexing and fiber-optic gyroscope |
CN116086507A (en) | 2022-12-16 | 2023-05-09 | 国网江苏省电力有限公司泰州供电分公司 | A phase quadrature four-wavelength optical fiber F-P cavity sensor demodulation system and method |
CN115791090B (en) * | 2023-02-08 | 2023-05-05 | 武汉昊衡科技有限公司 | System and method for improving signal measurement sensitivity and polarization stability |
CN116105777B (en) * | 2023-04-11 | 2023-07-11 | 广东海洋大学 | Quasi-distributed F-P interferometric optical fiber sensor and its signal demodulation method |
Citations (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5555086A (en) * | 1991-05-31 | 1996-09-10 | Litton Systems, Inc. | Coherence multiplexed interferometric signal processing system and method |
US5696857A (en) * | 1996-07-25 | 1997-12-09 | Litton Systems, Inc. | WDM/FDM fiber optic sensor architecture using WDM tap coupler |
CN201322623Y (en) * | 2008-11-21 | 2009-10-07 | 中国科学院上海光学精密机械研究所 | Embedded multi-channel high-speed fiber grating sensor demodulation system |
CN103115636A (en) * | 2013-02-06 | 2013-05-22 | 天津大学 | Optical fiber Fabry-Perot sensor multiplexing method and device based on multi-wavelength and low-coherence light source |
CN103940362A (en) * | 2014-04-30 | 2014-07-23 | 中国科学院半导体研究所 | High-precision fiber bragg grating low-frequency strain sensing demodulation system |
CN104931081A (en) * | 2015-06-10 | 2015-09-23 | 天津大学 | Composite wavelength reference-based fiber bragg grating sensing demodulation device and method |
CN106017519A (en) * | 2016-05-05 | 2016-10-12 | 重庆大学 | Optical fiber Fabry-Perot sensor demodulation system and method |
CN106525091A (en) * | 2016-10-25 | 2017-03-22 | 华中科技大学 | Fiber grating array sensing demodulation system based on multi-wavelength pulse differential modulation |
Family Cites Families (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US7336365B2 (en) * | 2005-02-11 | 2008-02-26 | Optoplan As | Method and apparatus for suppression of crosstalk and noise in time-division multiplexed interferometric sensor systems |
CN103438915A (en) * | 2013-09-11 | 2013-12-11 | 武汉理工大学 | F-P sensor multiplexing method and system based on frequency shift interference |
CN103512510B (en) * | 2013-10-23 | 2016-04-13 | 中国电子科技集团公司第三十四研究所 | Based on fiber grating sensing system and the operation method of narrow band scanning light source |
-
2018
- 2018-11-26 CN CN201811419299.9A patent/CN109520532B/en active Active
Patent Citations (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5555086A (en) * | 1991-05-31 | 1996-09-10 | Litton Systems, Inc. | Coherence multiplexed interferometric signal processing system and method |
US5696857A (en) * | 1996-07-25 | 1997-12-09 | Litton Systems, Inc. | WDM/FDM fiber optic sensor architecture using WDM tap coupler |
CN201322623Y (en) * | 2008-11-21 | 2009-10-07 | 中国科学院上海光学精密机械研究所 | Embedded multi-channel high-speed fiber grating sensor demodulation system |
CN103115636A (en) * | 2013-02-06 | 2013-05-22 | 天津大学 | Optical fiber Fabry-Perot sensor multiplexing method and device based on multi-wavelength and low-coherence light source |
CN103940362A (en) * | 2014-04-30 | 2014-07-23 | 中国科学院半导体研究所 | High-precision fiber bragg grating low-frequency strain sensing demodulation system |
CN104931081A (en) * | 2015-06-10 | 2015-09-23 | 天津大学 | Composite wavelength reference-based fiber bragg grating sensing demodulation device and method |
CN106017519A (en) * | 2016-05-05 | 2016-10-12 | 重庆大学 | Optical fiber Fabry-Perot sensor demodulation system and method |
CN106525091A (en) * | 2016-10-25 | 2017-03-22 | 华中科技大学 | Fiber grating array sensing demodulation system based on multi-wavelength pulse differential modulation |
Non-Patent Citations (2)
Title |
---|
Demodulation algorithm for optical fiber F-P sensor;HUADONG YANG et.al;《Applied Optics》;20170910;第56卷(第26期);第7450-7453页 * |
Multiplexing optical fiber displacement sensor based on heterodyne interference with frequency-modulated laser diode;Tian Qian, Zhang Enyao;《SPIE Digital Labrary》;19951231;第178-185页 * |
Also Published As
Publication number | Publication date |
---|---|
CN109520532A (en) | 2019-03-26 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN109520532B (en) | A multi-sensor multiplexing demodulation system and processing method of a fiber optic Faber sensor | |
CN107024236B (en) | F-P/FBG optical fiber sensor demodulation system | |
CN103604446B (en) | A kind of demodulation method of the multi-channel fiber Bragg grating absolute wavelength demodulating system based on simple detector | |
CN105606193A (en) | Optical fiber fabry-perot acoustic-vibration sensing device and demodulation method based on double tunable light sources | |
CN112697257B (en) | Non-fading multi-wavelength distributed acoustic wave sensing system and differential rotation vector superposition method | |
CN103115636B (en) | Optical fiber Fabry-Perot sensor multiplexing method and device based on multi-wavelength and low-coherence light source | |
CN106643522A (en) | Optical-fiber low-coherence interference displacement demodulation device and method based on photoelectric oscillator | |
CN102003944B (en) | Multi-scale quasi-distributed white light interference strain measurement device and method with common path compensation | |
US9658052B2 (en) | Method for reducing interference from scattered light/reflected light of interference path by generating carrier through phase | |
CN101532850B (en) | A method and device for fiber Bragg grating sensing demodulation | |
CN109238658B (en) | Method for measuring delay parameter of optical delay device | |
CN111397851A (en) | OFDR multi-path optical fiber sensing system and method based on optical frequency comb technology | |
CN101319919B (en) | A method and device for demodulating a frequency-domain fiber grating sensor network | |
CN105547336A (en) | Fiber grating sensing demodulation device and method on the basis of photoelectric oscillation loop | |
JP2021032734A (en) | measuring device | |
CN102003971B (en) | Method for eliminating backscattering light influence in optical fiber sensor | |
CN105806380A (en) | Multiplexing demodulation equipment based on long-cycle fiber grating reflective sensor | |
CN103438915A (en) | F-P sensor multiplexing method and system based on frequency shift interference | |
CN101271242A (en) | A method and device for demodulating a fiber grating sensor network | |
CN217466666U (en) | A multi-point gas detection device based on photothermal effect and wavelength division multiplexing interferometer | |
AU2020103490A4 (en) | A multiplexing optical fiber interferometer and its nesting construction method | |
CN117029995A (en) | High sensitivity vibration sensing system and method employing broadband light sources | |
CN207991566U (en) | A kind of double SLED optical fiber Fabry-Perot sensors demodulating equipments | |
CN207439428U (en) | Realize the demodulating equipment of fiber F-P and FBG sensor | |
US10024697B2 (en) | Method and system using wavelength division multiplexing for eliminating and reducing light diffusion and light reflection interference in interference path |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PB01 | Publication | ||
PB01 | Publication | ||
SE01 | Entry into force of request for substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
GR01 | Patent grant | ||
GR01 | Patent grant |